TECHNICAL FIELD
[0001] This invention relates to using a plasma fluorination treatment method to fluorinate
porous articles.
BACKGROUND
[0002] Plasma-deposited fluorocarbon coatings can impart desirable properties, such as low
surface energy, water-repellency, soil resistance, and durability, to a treated article.
A charge can be imparted to the treated article, which makes the article suitable
for use in items such as aerosol filters, face masks, air filters, and electrostatic
elements in electro-acoustical devices such as microphones, headphones, and electrostatic
recorders. Other surface modification techniques, such as those taught in US Pat.
No 5,437,900 include removal of surface fibrils but do not teach methods of fluorinating
porous article. Accordingly, plasma fluorination methods that can quickly and efficiently
produce an article with a fluorocarbon coating are desired.
SUMMARY OF INVENTION
[0003] One aspect of the present invention features a plasma fluorination method to fluorinate
porous articles, both on the surface and in the interior. It also features the resulting
articles.
[0004] One aspect of the present invention is a method of fluorinating a porous article
comprising: providing a reaction chamber having a capacitively-coupled system comprising
at least one grounded electrode and at least one electrode powered by an RF source;
generating a fluorine-containing plasma in the chamber thereby causing an ion sheath
to form adjacent to the electrodes; placing a porous article in the ion sheath of
the powered electrode; and allowing reactive species from the plasma to react with
the article surface and interior whereby the article becomes fluorinated.
[0005] Another aspect of the present invention is a method of fluorinating a porous article
comprising: providing a reaction chamber having a capacitively-coupled system comprising
at least one electrode powered by an RF source and at least one grounded electrode
that is substantially parallel to the surface of the powered electrode and separated
from the grounded electrode by about 25 millimeters or less; generating a fluorine-containing
plasma in the chamber at a pressure of about 40 Pascal or less; placing a porous article
between the substantially parallel electrodes and outside of the ion sheath; and allowing
reactive species from the plasma to react with the article surface and interior for
a total treatment time of over two minutes whereby the article becomes fluorinated.
[0006] Another aspect of the present invention is a method of fluorinating a porous article
comprising: providing a reaction chamber having a capacitively-coupled system comprising
at least one electrode powered by an RF source and at least one grounded electrode
that is substantially parallel to the surface of the powered electrode and separated
from the grounded electrode by about 25 millimeters or less; generating a fluorine-containing
plasma in the chamber thereby causing an ion sheath to form adjacent to the electrodes;
placing a porous article in the ion sheath of the grounded electrode; and allowing
reactive species from the plasma to react with the article surface and interior for
a total treatment time of about 30 seconds to about 5 minutes whereby the article
becomes fluorinated.
[0007] Another aspect of the present invention is a method of fluorinating a porous article
comprising: providing a reaction chamber having a capacitively-coupled system comprising
at least one electrode powered by an RF source and at least one grounded electrode
that is substantially parallel to the surface of the powered electrode and separated
from the grounded electrode by about 13 millimeters or less; generating a fluorine-containing
plasma in the chamber thereby causing an ion sheath to form adjacent to the electrodes;
placing a porous article between the electrodes; and allowing reactive species from
the plasma to react with the article surface and interior whereby the article becomes
fluorinated.
[0008] The methods may include embodiments wherein the process is continuous and/or wherein
the treatment time is less than about 60 seconds.
[0009] The porous article to be treated may be selected from the group consisting of foams,
woven materials, nonwoven materials, membranes, frits, porous fibers, textiles, and
microporous articles. The article may have pores smaller that the mean free path of
any species in the plasma. The article may have two parallel major surfaces and may
be treated on one or both major surface.
[0010] The methods may be carried out with the electrodes separated by 25 millimeters or
less. In some embodiments, the electrodes are separated by about 16 millimeters (mm)
or about 13 mm. Another aspect of the invention is an article comprising at least
one fluorinated porous layer having a basis weight of 10 to 300 gsm and a thickness
of 0.20 to 20 mm, wherein the layer has a Q
200 of greater than 1.1. The layer may have an effective fiber diameter of 1 to 50 µm.
[0011] Another aspect of the invention is an apparatus for fluorinating a substrate comprising
a vacuum chamber, a capacitively-coupled system within the chamber comprising at least
one electrode powered by an RF source and at least one grounded electrode substantially
parallel to the powered electrode wherein the electrodes are separated by 25 mm or
less, e.g., about 16 mm or 13 mm, and a means for generating a fluorine-containing
plasma throughout the entire chamber.
[0012] The powered electrode may comprise one or more rotating drums. The apparatus can
comprise an asymmetric parallel plate reactor.
[0013] As used in this invention:
"microporous membrane" means a membrane having pore sizes with a lower limit of 0.05
µm and an upper limit of 1.5 µm;
"plasma fluorocarbon" means a material deposited from a plasma comprising fluorocarbon
species;
"plasma fluorination" means thin film deposition, surface modification, and any other
plasma-induced chemical or physical reaction that can fluorinate an article;
"porous article" means an article having pathways open to at least one surface;
"Q200" means the quality factor rating of a filter; the procedure for determining Q200 is set forth in the Examples section of this application, and
"substantially parallel" means the electrodes are substantially the same distance
from each other along their entire lengths, including concentric electrodes.
[0014] An advantage of at least one embodiment of the present invention is that it provides
a continuous plasma fluorination method, which allows for efficient, i.e., faster,
processing of articles, especially continuous articles, e.g., long sheets of material,
as are used in roll-to-roll processing.
[0015] Another advantage of at least one embodiment of the invention is that it provides
a durable fluorination treatment through the bulk of porous articles, including microporous
membranes.
[0016] Another advantage of at least one embodiment of the present invention is that treatment
efficiencies can be obtained by placing the article to be treated within an ion sheath.
[0017] Another advantage of at least one embodiment of the present invention is that fluorination
efficiency may be achieved by reducing the space between the powered and grounded
electrode to 25 mm or less.
[0018] Other features and advantages of the invention will be apparent from the following
drawings, detailed description, and claims.
BRIEF DESCRIPTION OF DRAWINGS
[0019]
Fig. 1 depicts a parallel plate plasma apparatus for performing the plasma fluorination
of the present invention.
Fig. 2 depicts a single drum plasma apparatus for performing the plasma fluorination
of the present invention.
DETAILED DESCRIPTION
[0020] The present invention provides a plasma fluorination method to fluorinate a porous
article.
[0021] One method embodiment involves providing a reaction chamber having a capacitively-coupled
electrode system wherein an ion sheath is formed adjacent to at least one electrode
when a plasma is generated in the system. The ion sheath is an area adjacent to an
electrode in which ion bombardment is prevalent. The porous article to be treated
is placed within the ion sheath.
[0022] This method of the invention can be especially effective for articles with small
pores because the ion sheath can force chemical species from the plasma into small
pores of the articles being treated. This results in surprisingly fast fluorination
of the pore interiors. It was not expected that plasma fluorination could be achieved
within small pores, especially in cases where the pores are smaller than the mean
free path of any species in the plasma.
[0023] The mean free path (MFP) for a particular species is the average distance traveled
by a species before it collides with another species. The MFP depends in part on pressure
because the proximity of species influences the collision frequency. For example,
at 0.13 Pa (1 mTorr) and room temperature, the mean free path of an argon atom is
80 mm.
See Brian Chapman,
Glow Discharge Processes, 153 (John Wiley & Sons, New York 1980). Most other gases, including those used in
the present invention, are within three times (i.e. 26-240 mm) of this value at this
pressure. In the range of pressures useful for plasma fluorination, the mean free
path of argon varies from 80 mm to 0.08 mm (or 80 microns). Other gases would have
similar variations.
[0024] In plasma-treating a porous article, if the pore size is smaller than the mean free
path of the species in the plasma (i.e., smaller than 20 microns), normally the free
radical species generated in the plasma will collide with the pore walls near the
pore opening. The free radicals will react with molecules in the pore walls near the
pore opening rather than traveling into the depths of the pores. Therefore, one would
not expect the plasma fluorination to penetrate into the depths of the pores, especially
when the pores have tortuous paths.
[0025] Another method embodiment of the present invention involves providing a reaction
chamber having a capacitively-coupled electrode system in which a powered and grounded
electrode are spaced 25 mm (one inch), or less, apart and the porous article to be
treated is suspended between the two electrodes and outside an ion sheath. In this
embodiment, the chamber pressure is maintained at 40 Pa or less and the total treatment
time is over 2 minutes. This treatment method results in treated articles having a
higher fluorine content, and better oil repellency, than similar articles treated
in a system in which the grounded and powered electrode are farther apart and the
chamber pressure is higher than 40 Pa.
[0026] Another method embodiment of the present invention involves providing a reaction
chamber having a capacitively-coupled system comprising at least one electrode powered
by an RF source and at least one grounded electrode that is substantially parallel
to the surface of the powered electrode and separated from the grounded electrode
by 25 millimeters or less; generating a fluorine-containing plasma in the chamber
thereby causing an ion sheath to form adjacent to the electrodes; placing a porous
article in the ion sheath of the grounded electrode; and allowing reactive species
from the plasma to react with the article surface and interior for a total treatment
time of 30 seconds to 5 minutes whereby the article becomes fluorinated.
[0027] Another method embodiment of the present invention involves providing a reaction
chamber having a capacitively-coupled system comprising at least one electrode powered
by an RF source and at least one grounded electrode that is substantially parallel
to the surface of the powered electrode and separated from the grounded electrode
by 13 millimeters or less; generating a fluorine-containing plasma in the chamber
thereby causing an ion sheath to form adjacent to the electrodes; placing a porous
article between the electrodes; and allowing reactive species from the plasma to react
with the article surface and interior whereby the article becomes fluorinated.
Porous Articles
[0028] Porous articles suitable for use in the present invention include foams, nonwoven
materials, woven materials, membranes, frits, porous fibers, textiles, and microporous
articles. These articles may have pore sizes of 0.05 micrometers or greater.
[0029] The porous articles may be made from, e.g., polymers, metals, glasses, and ceramics.
Suitable polymers for the above articles include polyolefins such as, e.g., polypropylene,
polyethylene, poly-(4-methyl-1-pentene), and combinations thereof, halogenated vinylpolymers
(e.g., polyvinyl chloride), polystyrene, polycarbonates, polyesters, polyamides, and
combinations thereof. The nonwovens can be formed by a variety of methods, including
but not limited to, carding, use of a rando-webber, spunbonding, hydrolacing, or blown
microfibers. The textiles and cloths can be formed as nonwovens or as knit or woven
materials. The textiles and cloths preferably have a basis weight in the range of
10 to 500 grams per square meter more preferably 15 to 300 grams per square meter.
Porous frits synthesized from polymers, metals, glasses and ceramics are available
commercially in various pore sizes. The pore size typically varies between 1 and 250
microns and the frits may have a void volume of between 20 and 80%. Typical applications
of frits include filtration, support media for membrane cartridges, solvent filters,
diffusers, fluidization supports, bio-barriers, nibs for writing instruments, chromatographic
support media, and catalysis support media. Porous fibers are also commercially available.
Typical diameters for these fibers are up to and around 100 µm and typical pore sizes
are from 0.001 1µm (10 Å) to 10 µm (1000 Å).
[0030] Suitable microporous films may be prepared by thermally-induced phase separation
(TIPS) methods such as those described in U.S. Patent Nos. 4,539,256 (Shipman), 4,726,989;
5,120,594 (Mrozinski); and 5,260,360 (Mrozinski et al.) which describe such films
containing a multiplicity of spaced, randomly dispersed, equiaxed, nonuniform shaped
particles of a thermoplastic polymer. These films typically have pore sizes with a
lower limit of 0.05 micrometers and an upper limit of 1.5 micrometers.
[0031] A suitable porous material may have a basis weight of 10 to 300 gsm (grams per square
meter) and a thickness of 0.20 to 20 mm. The porous material also may have an effective
fiber diameter of 1 to 50 µm.
[0032] The porous articles can be any shape, e.g., sheets, rods, and cylinders, as long
as they can be placed within an ion sheath that surrounds an electrode. Typically
the articles will be sheet-like with two major parallel surfaces. The articles may
be discrete articles or may be continuous sheets of material. They may have any level
of hydrophobicity or hydrophilicity before they are treated.
[0033] The resulting fluorinated porous article may be used alone or may be incorporated
into another article. For example, it may be incorporated into a multi-layer (two
or more layers) article in which the other layer(s) are fluorinated or unfluorinated
and are porous or nonporous. The multi-layer article may be made by any method known
in the art, e.g., lamination, and physical bonding.
[0034] Porous filter media are frequently employed to filter air containing solid and/or
liquid particles. The particles removed are often toxic or noxious substances. Scientists
and engineers have long sought to improve filtration performance of air filters. Some
of the most effective air filters use electret articles. Electrets are dielectric
articles that exhibit a lasting charge, that is, a charge that is at least quasi-permanent.
The term "quasi-permanent" means that the time constants characteristic for the decay
of the charge are much longer than the time period over which the electret is used.
[0035] The charged nature of the electret enhances the filter's ability to attract and retain
particles such as dust, dirt, and fibers that are present in the air. Electrets have
been found to be useful in a variety of applications including air, furnace and respiratory
filters, face masks, and electro-acoustic devices, such as microphones, headphones,
and electrostatic recorders.
[0036] Over the years, various methods of making and improving the filtration performance
of nonwoven fibrous electrets have been developed. These methods include, e.g., bombarding
fibers with electrically charged particles as the fibers issue from a die orifice,
corona charging a nonwoven fibrous web, and hydrocharging a nonwoven fibrous web.
[0037] While performance is enhanced through the use of electret charged media, degradation
in filter efficiency during exposure or loading of aerosols containing an oily mist
has been exhibited in some media. This change in performance during loading prompted
the National Institute for Occupational Safety and Health (NIOSH) to specify testing
that requires respirators used in oily mist environments to be exposed to 200 mg of
dioctyl phthalate (DOP) during certification testing. In order to determine the benefits
of the filters of this invention, the filter penetration was measured after exposing
the sample to 200 mg of aerosolized DOP.
[0038] In addition to penetration, pressure drop of the filter is a key measurement in designing
a filter. Pressure drop is defined as a reduction in static pressure within an air
stream between the upstream and downstream sides of a filter through which the air
stream passes. A lower pressure drop allows air to flow through the medium more easily.
Lower pressure drop is typically preferred because it allows less effort or energy
to be used to achieve the desired flow. This is true whether the filter is employed
as a respirator, which a user breathes through; a battery powered air-purifying respirator,
or a home furnace filter.
[0039] To ease the comparison and the design of filters, researchers often combine penetration
and pressure drop into a single term of Quality Factor, i.e., the quality of the filtration
performance of the material. In this application, quality factor is based on penetration
and pressure drop after exposure to of 200 mg of dioctyl phthalate, as explained in
more detail in the Examples section. The Quality Factor Rating is referred to as Q
200.
[0040] Some articles of the present invention have Q
200 ratings over 1.1, and in some cases, as high as 1.53. Some articles also have fluorine
concentrations of over 3700 ppm, and in some cases, as high as 5000 ppm or more.
Apparatus
[0041] An apparatus suitable for the present invention provides a reaction chamber having
a capacitively-coupled system with at least one electrode powered by an RF source
and at least one grounded electrode. In some embodiments, a grounded electrode is
separated from the powered electrode by 25mm or less.
[0042] A suitable reaction chamber is evacuable, has means for generating a fluorinated
plasma throughout the entire chamber and is capable of maintaining conditions that
produce plasma fluorination. That is, the chamber provides an environment which allows
for the control of, among other things, pressure, the flow of various inert and reactive
gases, voltage supplied to the powered electrode, strength of the electric field across
the ion sheath, formation of a plasma containing reactive species, intensity of ion
bombardment, and rate of deposition of a film from the reactive species. Aluminum
is a preferred chamber material because it has a low sputter yield, which means that
very little contamination occurs from the chamber surfaces. However, other suitable
materials, such as graphite, copper, glass or stainless steel, maybe used.
[0043] The electrode system may be symmetric or asymmetric. Preferred electrode surface
area ratios between grounded and powered electrodes for an asymmetric system are from
2:1 to 4:1, and more preferably from 3:1 to 4:1, The ion sheath on the smaller powered
electrode will increase as the ratio increases, but beyond a ratio of 4:1 little additional
benefit is achieved. Placing the sample on the powered electrode is generally preferred
because DC bias would not be shunted to ground. Both electrodes may be cooled, e.g.,
by water.
[0044] Plasma, created from the gas within the chamber, is generated and sustained by supplying
power (for example, from an RF generator operating at a frequency in the range of
0.001 to 100 MHz) to at least one electrode. The RF power source provides power at
a typical frequency in the range of 0.01 to 50 MHz, preferably 13.56 MHz or any whole
number (e.g., 1, 2, or 3) multiple thereof. The RF power source can be an RF generator
such as a 13.56 MHz oscillator. To obtain efficient power coupling (i.e., wherein
the reflected power is a small fraction of the incident power), the power source may
be connected to the electrode via a network that acts to match the impedance of the
power supply with that of the transmission line (which is usually 50 ohms resistive)
so as to effectively transmit RF power through a coaxial transmission line. A description
of such networks can be found in Brian Chapman,
Glow Discharge Processes, 153 (John Wiley & Sons, New York 1980). One type of matching network, which includes
two variable capacitors and an inductor, is available as Model # AMN 3000 from RF
Power Products, Kresson, NJ. Traditional methods of power coupling involve the use
of a blocking capacitor in the impedance matching network between the powered electrode
and the power supply. This blocking capacitor prevents the DC bias voltage from being
shunted out to the rest of the electrical circuitry. On the contrary, the DC bias
voltage is shunted out to the grounded electrode. While the acceptable frequency range
from the RF power source may be high enough to form a large negative DC self bias
on the smaller electrode, it should not be so high that it creates standing waves
in the resulting plasma, which is inefficient for plasma fluorination.
[0045] The articles to be treated may be placed in, or passed through, the evacuable chamber.
In some embodiments, a multiplicity of articles may be simultaneously exposed to the
plasma during the process of this invention.
[0046] In an embodiment in which the article is treated within an ion sheath, plasma fluorination
of discrete planar articles can be achieved, for example, by placing the articles
in direct contact with the powered electrode. This allows the article to act as an
electrode due to capacitive coupling between the powered electrode and the article.
This is described in M. M. David, et al.,
Plasma Deposition and Etching of Diamond-Like Carbon Films, AIChE Journal, vol. 37, No. 3, p. 367 (1991). In the case of an elongated article,
the article may optionally be pulled through the vacuum chamber continuously, while
maintaining contact with an electrode. The result is a continuous plasma fluorination
of the elongated article.
[0047] Figure 1 illustrates a parallel plate apparatus 10 suitable for the present invention,
showing a grounded chamber 12 from which air is removed by a pumping stack (not shown).
Gases to form the plasma are injected radially inward through the reactor wall to
an exit pumping port in the center of the chamber. Article 14 is positioned proximate
RF-powered electrode 16. Electrode 16 is insulated from chamber 12 by Teflon support
18.
[0048] It is not necessary to confine the plasma between the electrodes. The plasma may
fill the entire chamber without diminishing the effectiveness of the plasma fluorination.
However, the plasma will usually appear brighter between the two electrodes.
[0049] Figure 2 illustrates single-drum apparatus 100 that is also suitable for the present
invention, especially the method embodiment that employs an ion sheath. This apparatus
is described in more detail in U.S. Pat. No. 5,948,166. The primary components of
apparatus 100 are rotating drum electrode 102 that can be powered by a radio frequency
(RF) power source, grounded chamber 104 that acts as a grounded electrode, feed reel
106 that continuously supplies article 108, which is to be treated, and a take-up
reel 110, which collects the treated article. A concentric grounded electrode (not
shown) can be added near the powered electrode so spacing can be controlled.
[0050] Article 108 is a long sheet that, in operation, travels from feed reel 106, around
drum electrode 102 and on to take-up reel 110. Reels 106 and 110 are optionally enclosed
within chamber 104, or can be outside chamber 104 as long as a low-pressure plasma
can be maintained within the chamber.
[0051] The curvature of the drum provides intimate contact between the article and the electrode,
which ensures that the article remains within the ion sheath, irrespective of other
operating conditions such as pressure. This can allow a thick article to be kept within
the ion sheath even at high pressures (e.g., 300 to 1000 mTorr). Because the article
is supported and carried by the drum, this intimate contact also enables the treatment
of delicate materials. The intimate contact also ensures that plasma fluorination
is captured by the article, thereby keeping the electrode clean. It also allows for
effective single-sided treatment when this is desired. However, dual-sided treatment
can be achieved by passing the article through the apparatus twice, with one side
being treated per pass. A drum electrode also provides a long treatment zone (pi x
diameter) and provides symmetric distribution of power across the electrode, which
can have operational advantages. The drum may be cooled or heated to control the temperature
of the article being treated. In addition, linear dimensions in the direction of current
flow are made small in comparison to the wavelength of the RF radiation, eliminating
the problem of standing waves.
[0052] In other suitable apparatuses, there may be more than one powered electrode and more
than one grounded electrode. One suitable apparatus for this invention is a reactor
comprising two drum shaped powered electrodes within a grounded reaction chamber,
which has two to three times the surface area of the powered electrodes. The drums
can be configured so that the article to be treated can travel around and over the
two drums in a manner that allows it to be plasma-treated on both sides (one side
is treated on each drum). The drums may be located in a single chamber or in separate
chambers, or may be in the same chamber, but separated, such that different treatments
can occur around each drum.
[0053] When multiple electrodes are used, they may be powered by a single RF supply or powered
separately. When a single supply is used, the power is sometimes distributed unequally
between the electrodes. This may be corrected by using a different power supply for
each electrode with oscillator circuits linked to a master power supply through a
phase angle adjuster. Thus any power coupling between the electrodes through the plasma
may be fine-tuned by adjusting the phase angle between the voltage waveforms of the
master and slave power supplies. Flexibility in power coupling and adjustment between
the different electrodes may be achieved by this approach.
[0054] In some embodiments, it is desirable to have the grounded electrode within about
25 mm of the powered electrode on which an article to be treated is located. Having
a grounded electrode close to a powered electrode was found to be advantageous. It
resulted in articles with high levels of fluorination and oil repellency. It was further
found that, while the proximity of the electrodes provided advantages, it was not
necessary that the plasma be restricted to the area between the electrodes. While
the plasma glow tended to be brighter between the electrodes, the plasma filled the
entire reaction chamber. In addition, one experiment was carried out in which the
grounded electrode was perforated to more clearly show that the plasma was not confined.
The properties of the resulting article were as good as those of articles produced
with an unperforated electrode.
[0055] In addition to the capacitive coupling system, the reactor might include other magnetic
or electric means such as induction coils, and grid electrodes.
Methods of Plasma Fluorination
[0056] Other aspects of the invention are further directed to methods of plasma-treating
articles. The methods are carried out in a suitable capacitively coupled reactor system
such as those described above.
[0057] In different embodiments of methods of the present invention, a grounded and a powered
electrode are spaced apart by 25 mm or less, 16 mm or less, or 13 mm or less. A low
chamber pressure may be used and can be beneficial in some embodiments because the
lower pressure normally allows bigger ion sheaths to form. An article to be treated
may be placed on the powered electrode (preferably), the grounded electrode, or may
be suspended between the electrodes. Plasma fluorination of discrete planar articles
can be achieved, for example, by suspending an article between the electrodes, preferably
about halfway between the electrodes. In this embodiment, the article may be, but
does not need to be, within an ion sheath. If the article is outside of an ion sheath,
e.g., by being suspended, a treatment time of over two minutes may be required to
deposit a fluorinated layer with good oil repellency properties. However, reducing
the space between the electrodes, e.g., to about 16 mm or about 13 mm, can decrease
the necessary treatment time. Total treatment times of less than two minutes can be
achieved if the article is within an ion sheath.
[0058] The article to be treated optionally may be pre-cleaned by methods known to the art
to remove contaminants that may interfere with the plasma fluorination. A useful pre-cleaning
method is exposure to an oxygen plasma. For this pre-cleaning, pressures in the reactor
are maintained between 1.3 Pa (10 mTorr) and 27 Pa (200 mTorr). Plasma is generated
with RF power levels of between 500 W and 3000 W. Other gases maybe used for pre-cleaning
such as, for example, argon, air, nitrogen, hydrogen or ammonia, or mixtures thereof.
[0059] Prior to the plasma fluorination process, the chamber is evacuated to the extent
necessary to remove air and any impurities. This may be accomplished by vacuum pumps
at a pumping stack connected to the chamber. Inert gases (such as argon) may be admitted
into the chamber to alter pressure. Once the chamber is evacuated, a source gas containing
fluorine is admitted into the chamber via an inlet tube. The source gas is introduced
into the chamber at a desired flow rate, which depends on the size of the reactor,
the surface area of the electrodes, and the porosity of the articles to be treated.
Such flow rates must be sufficient to establish a suitable pressure at which to carry
out plasma fluorination, typically 0.13 Pa to 130 Pa (0.001 Torr to 1.0 Torr). For
a cylindrical reactor that has an inner diameter of approximately 55 cm and a height
of approximately 20 cm, the flow rates are typically from 50 to 500 standard cubic
centimeters per minute (sccm), At the pressures and temperatures of the plasma fluorination
(typically 0.13 to 133 Pa (0.001 to 1.0 Torr) (all pressures stated herein are absolute
pressures) and less than 50°C), the source gases remain in their vapor form.
[0060] Upon application of an RF electric field to a powered electrode, a plasma is established.
In an RF-generated plasma, energy is coupled into the plasma through electrons. The
plasma acts as the charge carrier between the electrodes. The plasma can fill the
entire reaction chamber and is typically visible as a colored cloud.
[0061] The plasma also forms an ion sheath proximate at least one electrode. In an asymmetric
electrode configuration, higher self-bias voltage occurs across the smaller electrode.
This bias is generally in the range of 100 to 2000 volts. This biasing causes ions
within the plasma to accelerate toward the electrode thereby forming an ion sheath.
The ion sheath appears as a darker area adjacent to the electrode. Within the ion
sheath accelerating ions bombard species being deposited from the plasma onto, and
into, the porous article.
[0062] The depth of the ion sheath normally ranges from approximately 1mm (or less) to 50
mm and depends on factors such as the type and concentration of gas used, pressure
in the chamber, the spacing between the electrodes, and relative size of the electrodes.
For example, reduced pressures will increase the size of the ion sheaths. When the
electrodes are different sizes, a larger (i.e., stronger) ion sheath will form adjacent
to the smaller electrode. Generally, the larger the difference in electrode size,
the larger the difference in the size of the ion sheaths. Also, increasing the voltage
across the ion sheath will increase ion bombardment energy.
[0063] The article to be treated is placed on or near at least one electrode in the reaction
chamber. In the case of an elongated article, the article optionally may be pulled
through the vacuum chamber continuously. Contact with an electrode does not need to
be maintained. The fluorine species within the plasma react on the article's surface
and interior. A suitable plasma could contain fluorine and one or more of oxygen,
carbon, sulfur, and hydrogen in various combinations and ratios. The degree of fluorination
of the final article may be controlled by a number of factors, for example, the components
of the plasma, the length of treatment, and the partial pressure of the plasma components.
The plasma fluorination results in species in the plasma becoming randomly attached
to the article surface (including interior surfaces) via covalent bonds. The deposited
fluorine composition may constitute a full layer over the entire exposed article surface
(including interior surfaces), may be more sparsely distributed on the article, or
may be deposited as a pattern through a shadow mask.
[0064] Sources of fluorine include compounds such as carbon tetrafluoride (CF
4), sulfur hexafluoride (SF
6), C
2F
6, C
3F
8, and isomeric forms of C
4F
10 and C
5F
12, as well as hexafluoropropylene (HFP) trimer (a mixture of perfluoro 2,3,5 trimethyl
3-hexene; perfluoro 2,3,5-trimethyl 2-hexene; and perfluoro 2,4,5-trimethyl 2-hexene,
available from 3M Company).
[0065] Other plasma fluorinations might include deposition of amorphous films of containing
fluorine such as aluminum fluoride, copper fluoride, fluorinated silicon nitride,
silicon oxyfluorides, and. Furthermore, these might include the attachment of additional
functional groups.
[0066] For treatments with carbon- or carbon-and-hydrogen-rich plasma fluorinations, hydrocarbons
are particularly preferred as sources. Suitable hydrocarbon sources include acetylene,
methane, butadiene, benzene, methylcyclopentadiene, pentadiene, styrene, naphthalene,
and azulene. Mixtures of these hydrocarbons may also be used. Another source of hydrogen
is molecular hydrogen (H
2). Sources of oxygen include oxygen gas (O
2), hydrogen peroxide (H
2O
2), water (H
2O), nitrous oxide (N
2O), and ozone (O
3).
[0067] When treatment comprises deposition of a film, it typically occurs at rates ranging
from 1 to 100 mn/second (10 to 1000 Angstrom per second (A/sec)), depending on conditions
including pressure, power, concentration of gas, types of gases, and relative size
of electrodes. In general, deposition rates increase with increasing power, pressure,
and concentration of gas, but the rates will approach an upper limit.
[0068] The articles also may be treated in a manner to provide different degrees of fluorination
in different areas of the article. This can be achieved, for example, by using contact
masks to selectively expose portions of the porous article to the plasma fluorination.
The mask may be attached to the article or may be a separate web that moves with the
article. By this method, it is possible to obtain fluorinated areas on an article.
The fluorinated areas may be in any shape that can be achieved using a shadow mask,
e.g., circles, and stripes.
[0069] Articles having fluorination gradients may also be produced. This can be achieved
by exposing different areas of an article to the plasma fluorination treatment for
different lengths of time.
[0070] In the foregoing description, certain terms have been used for brevity, clarity,
and understanding. No unnecessary limitations are to be implied therefrom beyond the
requirement of the prior art because such terms are used for descriptive purposes
and are intended to be broadly construed. Moreover, the description and illustration
of the invention is by way of example, and the scope of the invention is not limited
to the exact details shown or described.
EXAMPLES
[0071] This invention may be illustrated by way of the following examples including the
described test methods used to evaluate and characterize the plasma fluorinated films
produced in the examples.
Plasma Reactor
[0072] A parallel-plate capacitively coupled plasma reactor (commercially available as Model
2480 from PlasmaTherm of St. Petersburg, Florida), typically used for reactive ion
etching, was used to carry out plasma treatments. The reactor had a chamber that was
cylindrical in shape with an internal diameter of 762 mm (30 inches) and height of
150 mm (6 inches) and a circular powered electrode having a diameter of 686 mm (27
inches) mounted inside the chamber. The powered electrode was attached to a matching
network and a 3 kW RF power supply that was operated at a frequency of 13.56 MHz.
The chamber was vacuum pumped with a Roots blower backed by a mechanical pump. Unless
otherwise stated, the base pressure in the chamber was about 1.3 Pa (10 mTorr) or
less. Process gases were metered into the chamber either through mass flow controllers
or a needle valve. Pressure was controlled independently from flowrate by a butterfly
valve. Unless otherwise stated, all the plasma treatments were done with the sample
located on the powered electrode of the plasma reactor. The samples were taped to
the electrode or secured with a metal frame.
Hydrocharging
[0073] Some samples were hydrocharged before testing. Hydrocharging can enhance filtration
performance of an article by imparting a permanent charge. Hydrocharging, as taught
in U.S. Pat. No. 5.496.507, imparts a permanent charge onto a media to enhance filtration.
This method of hydrocharging comprises impinging jets of water or a stream of water
droplets onto the sample at a pressure sufficient to provide the sample with filtration
enhancing electret charge. Samples were placed on a mesh belt support and moved at
a belt speed of approximately 4 inches/second (10.2 cm/sec) through water jets generated
by a pump-assisted water sprayer operating at a water pressure of 827 kPa (6206 Torr).
The water jets were positioned about 15 cm (6 in) above the belt. Water was simultaneously
removed from the sample by vacuum. Both sides of the samples were treated.
[0074] The sample was then passed two additional times over a vacuum to remove additional
moisture and then allowed to air-dry overnight before proceeding with testing.
Test Methods
DOP Penetration and Pressure Drop Test
[0075] Dioctyl phthalate (DOP) loading is a direct measurement of the resistance of a filter
medium to degradation due to exposure to an oily mist aerosol. The penetration through,
and the pressure drop across, a sample were monitored during prolonged exposure of
the sample to a DOP aerosol under specified conditions. Standard equipment and test
procedures were used for measuring filter performance.
[0076] The measurements were made using an automated filter tester (AFT) Model 8130 available
from TSI Incorporated, St. Paul, Minnesota that was set up with an oil aerosol generator.
DOP % Penetration was calculated automatically by the AFT instrument.

where the concentrations upstream and downstream were measured by light scattering.
The DOP aerosol generated by the AFT instrument was nominally monodisperse with a
mass median diameter of 0.3 micrometers and had an upstream concentration of 85 mg/m
3 to 110 mg/m
3 as measured using a gravimetric filter. Measurements were performed with the aerosol
neutralizer turned off and a flow rate through the sample of 42.5 liters per minute
(L/min), unless otherwise indicated.
[0077] Samples were tested in the following manner. Samples were cut and mounted in a sample
holder such that an 11.45 cm (4.5 inch) diameter portion of the sample was exposed
to the aerosol. The face velocity was 6.9 centimeters/second (cm/sec). Each test was
continued until the exposure on the sample was exposed to 200 mg DOP. The DOP % Penetration
and corresponding Pressure Drop data were determined by the AFT and transmitted to
an attached computer where the data was stored.
Quality Factor
[0078] Quality Factor (Q Factor) is a measurement of filtration performance. It depends
on the aerosol used, aerosol flow rate, and filter area. The Quality Factor of a sample
was calculated by the following formula:

where Q is in inverse mm H
2O units and Pressure Drop is in mm H
2O units. Q Factors were reported for a DOP penetration loading of 200 mg DOP (Q
200) at a flow rate of 42.5 L/min and a filter diameter of 11.4 cm resulting in a filter
area of 103 cm
2.
[0079] The higher the Q
200, the better the filtration performance.
Oil Repellency Test
[0080] Porous samples were evaluated for oil repellency using 3M Oil Repellency Test III
(February 1994), available from 3M. In this test, samples were challenged to either
penetration or droplet-spread by oil or oil mixtures having varying surface tensions.
Oils and oil mixtures were given a rating corresponding to the following:
| Oil Repellency Rating Number |
Oil Composition |
Surface Tension dynes/cm |
| 0* |
-- |
--- |
| 1 |
KAYDOL mineral oil |
31 |
| 2 |
65/35 (vol) mineral oil/n-hexadecane |
28 |
| 3 |
n-hexadecane |
26.5 |
| 4 |
n-tetradecane |
25.5 |
| 5 |
n-dodecane |
24 |
| 6 |
n-decane |
22 |
| 7 |
n-octane |
20.5 |
| 8 |
n-heptane |
18.5 |
| * fails KAYDOL mineral oil |
[0081] In running the Oil Repellency Test, a porous sample was placed on a flat, horizontal
surface. A small drop of oil composition was gently placed on the sample. If, after
ten seconds it was observedthat the drop was visible as a sphere or a hemisphere,
the porous sample is deemed to pass the test. The reported oil repellency rating of
the sample corresponds to the highest numbered oil or oil mixture thatwas repelled.
It was desirable to have an oil repellency rating of at least 1, preferably at least
3.
Fluorine Content
[0082] A sample size of about 1 to 3 mg was loaded into an Antek 9000F Fluoride Analysis
System available from Antek Instruments, Houston, Texas. The analysis was based on
oxypyrohydrolysis followed by final analysis with a fluoride ion specific electrode
(ISE). The carbon-fluorine bond was oxypyrohydrolyzed at 1050°C. The product hydrogen
fluoride (HF) is trapped in a buffer solution. The dissociated fluoride ions were
measured with fluoride ISE at a controlled temperature. The calibration curve was
based on standards prepared with FC-143 (C
7F
15CO
2NH
4) in the range of 25 ppm fluorine to 1000 ppm fluorine at an injection of from 10
to 15 µL.
Example 1
[0083] This example illustrates the effect of the combination of an ion sheath and electrode
spacing on Quality Factor (Q-Factor).
[0084] A blown microfiber porous article was made from propylene (available as EOD97-13
from ATOFINA Petrochemical, Houston, TX) that was extruded at a temperature of 350°C
and blown horizontally onto a collector at a distance of about 300 mm (12 in) from
the extruder. The resulting porous article had an effective fiber diameter 7.5 µm
as described in C.N. Davies, "Air Filtration" Academic Press, 1973. It also had a
solidity of 7.7%, a basis weight of 87.5 g/m
2, an effective pore diameter of 25 µm, and a thickness of about 1.24 mm (49 mils).
Web thickness was measured according to ASTM D1777-64 using a 230 g weight on a 10
cm diameter disk. In DOP Penetration testing at 42.5 L/min flow of DOP aerosol, the
article exhibited a pressure drop of 40 Pa (300 mTorr).
[0085] The porous article was cut into rectangles of about 15 cm x 30 cm used as samples
A to R. The samples were treated on the powered electrode in the Plasma Reactor with
plasma formed from perfluoropropane (C
3F
8) gas available from 3M Company and with various electrode separation distances and
process conditions as shown in Table 1. The reactor chamber was pumped down to a base
pressure of less than 1.3 Pa (10 mTorr). C
3F
8 was introduced into the chamber at a flow rate of 100 or 200 sccm. Chamber pressure
and radio frequency (RF) power were established. A bright plasma was seen in the inter-electrode
space and an ion sheath, which was darker than the plasma, formed adjacent to the
powered electrode and encompassed the porous article. For each sample the plasma treatment
was continued for one minute. Then the plasma was extinguished, the gas flow was stopped,
the chamber pressure brought down to below 1.3 Pa (10 mTorr), and the chamber was
vented to atmosphere. The sample was flipped over and the treatment was repeated on
the other side.
[0086] Samples were hydrocharged and measured for DOP penetration. The DOP Penetration Test
was run as described in the Test Method section above except the flow rate was 85
L/min and the neutralizer was on. Quality Factors, Q
200, are reported in Table 1.
Table 1
| Sample |
Spacing (mm) |
Power (W) |
Pressure (Pa) |
Flow (sccm) |
Q200 (at 85 L/min) |
| 1-A |
152 |
1500 |
37 |
100 |
0.398 |
| 1-B |
152 |
1000 |
67 |
200 |
0.086 |
| 1-C |
152 |
2000 |
67 |
200 |
0.120 |
| 1-D |
152 |
1000 |
13 |
100 |
0.441 |
| 1-E |
152 |
2000 |
13 |
100 |
0.335 |
| 1-F |
152 |
1500 |
37 |
100 |
0.309 |
| 1-G |
76 |
1500 |
37 |
100 |
0.358 |
| 1-H |
76 |
1000 |
67 |
200 |
0.094 |
| 1-I |
76 |
2000 |
67 |
200 |
0.124 |
| 1-J |
76 |
1000 |
13 |
100 |
0.445 |
| 1-K |
76 |
2000 |
13 |
100 |
0.422 |
| 1-L |
76 |
1500 |
40 |
100 |
0.428 |
| 1-M |
25 |
1500 |
37 |
100 |
0.574 |
| 1-N |
25 |
1000 |
67 |
200 |
0.376 |
| 1-O |
25 |
2000 |
67 |
200 |
0.556 |
| 1-P |
25 |
1000 |
13 |
100 |
0.582 |
| 1-Q |
25 |
2000 |
13 |
100 |
* |
| 1-R |
25 |
1500 |
40 |
100 |
0.570 |
| * This condition did not run with a stable plasma. |
[0087] The benefit of reducing the electrode spacing was clearly seen in the Q
200 values shown above.
Example 2 and Comparative Example 1
[0088] This example illustrates the effect of reduced electrode distance on Quality Factor
at the standard test conditions (i.e., 42 L/min and neutralizer off).
[0089] Example 2 was made as Example 1-D except a different electrode distance, chamber
pressure, and standard test conditions were used as described herein. The electrode
spacing was 0.625 in (16 mm) and chamber pressure was at 6.7 Pa (50 mTorr). The sample
was exposed to the plasma for two minutes on each side. The sample was measured for
Oil Repellency. The Oil Repellency Rating was 5. The sample was also hydrocharged
and measured for DOP penetration. Q
200 for this sample was 1.53.
[0090] Comparative Example 1 was made as Example 2 (except the electrode spacing was 76
mm). The sample was hydrocharged and measured for DOP penetration. Q
200 for this sample was 0.58.
[0091] The results show that decreasing the electrode spacing provides improved Q
200 qualities.
Example 3 and Comparative Example 2
[0092] This example illustrates the effect of plasma fluorination within an ion sheath on
the oil-repellency characteristics of a porous article.
[0093] Example 3 was made as Example 1-D except a different electrode distance, chamber
pressure, and standard test conditions were used as described herein. The electrode
spacing was 0.625 in (16 mm) and chamber pressure was at 16.6 Pa (125 mTorr). The
sample was exposed to the plasma for one minute on each side.
[0094] Comparative Example 2 was made in a manner similar to Example 3 except the porous
article was suspended in the plasma between the powered electrode and the grounded
electrode and about 8 mm from either electrode and thus outside the ion sheath. Because
a plasma existed on both sides of the suspended sample, the sample did not have to
be flipped over. Total treatment time was two minutes.
[0095] Example 3 and Comparative Example 1 were measured for oil repellency. The Oil Repellency
Rating for Example 3 and Comparative Example 1 were 5 and 4, respectively. The samples
were also hydrocharged and measured for DOP penetration. Quality Factors were determined
at different amounts of DOP penetration. The results are shown in Table 2.
Table 2
| DOP Penetration |
Quality Factor |
| |
Example 3 |
Comp. Example 2 |
| 0 |
2.59 |
1.52 |
| 20 |
2.30 |
1.22 |
| 40 |
2.10 |
1.02 |
| 60 |
1.93 |
0.84 |
| 80 |
1.83 |
0.73 |
| 100 |
1.72 |
0.62 |
| 120 |
1.61 |
0.54 |
| 140 |
1.51 |
0.46 |
| 160 |
1.44 |
0.40 |
| 180 |
1.37 |
0.35 |
| 200 |
1.28 |
0.23 |
[0096] As seen in the above table, the Quality Factor at 200 mg of DOP loading was 1.28
for Example 3. In contrast, the quality factor of Comparative Example 2 was 0.23.
The Q Factor results indicate that plasma fluorination of a porous sample within an
ion sheath was more efficient than plasma fluorination outside an ion sheath.
Example 4 and Comparative Example 3
[0097] This example illustrates the effect of exposure time and electrode distance on a
porous article treated outside of an ion sheath.
[0098] Example 4 was made as Comparative Example 2 except the total treatment time for the
sample was 4 minutes. The resulting sample had an Oil Repellency Rating of 4. The
sample was hydrocharged and measured for DOP Penetration. A Q
200 value of 1.28 was obtained.
[0099] Comparative Example 3 was made as Example 4. It was made outside an ion sheath with
an electrode spacing of 76 mm and for a total treatment time of 4 minutes. The sample
was hydrocharged and measured for DOP penetration. A Q
200 value of 0.48 was obtained.
Example 5
[0100] This example illustrates the effect of plasma fluorination on the oil-repellency
of a porous membrane having small pores.
[0101] Example 5 was made as Example 1-D except the porous article was different and and
electrode spacing and chamber pressure were changed. The porous article was a microporous
polyethylene membrane made according to U.S. Pat. No. 4,539,256 Ex 8 except the film
was stretched to 6 times its original length in one direction. The membrane had pore
diameters of about 0.09 micrometer. The electrode distance was about 16 mm (0.625
in) and the chamber pressure was 67 Pa (500 mTorr). The sample was exposed to the
plasma for about one minute on each side. The resulting treated sample had an Oil
Repellency Rating of 4. The Oil Repellency Rating of the untreated sample was 0.
Example 6
[0102] This example illustrates the effect of short exposure times on the oleophobicity
of a porous article.
[0103] Example 6 was made as Example 1-D except the electrode distance was 16 mm, the chamber
pressure was 67 Pa (500 mTorr), the total exposure times were less than 60 seconds,
and the conditions shown in Table 4 were used. The repellency rating of the untreated
sample was 0.
[0104] Both samples were tested for oil repellency and DOP penetration. Results are shown
in Table 3.
Table 3
| Sample |
Total Time (sec) |
Power (W) |
Pressure (Pa) |
Flow (sccm) |
Repel. Rating |
Q200 |
| 6-A |
20 |
1000 |
67 |
100 |
5 |
1.17 |
| 6-B |
10 |
1000 |
67 |
100 |
4 |
0.80 |
[0105] As shown above, Q
200 was over 1.1 at treatment time of 20 seconds.
Example 7
[0106] This example shows the effect of treatment time and proximity to an ion sheath on
treatment effect.
[0107] The samples each consisted of a four-layer stack of the polypropylene blown microfiber
webs. Each layer was made from polypropylene (available as EOD97-13 from ATOFINA Petrochemical)
that was extruded at a temperature of 330°C with a collector distance of about 300
mm (12 in). The resulting web had an effective fiber diameter of 7.0 µm, pressure
drop of 5.9 Pa (44 mTorr), a solidity of 4.7%, a basis weight of 15 g/m
2 and thickness of about 340 µm (13.5 mils). Each sample stack was treated with a C
3F
8 plasma in a manner similar to Example 1 but at various exposure times and with an
electrode separation distance of 16 mm (0.625 in). Two samples were made at each of
three different exposure times, 20 seconds, 120 seconds, and 240 seconds. For each
exposure time, one four-layer sample was positioned on the lower, powered electrode
(within an ion sheath) and a second four-layer sample was simultaneously positioned
approximately midway between the powered and grounded electrodes (outside an ion sheath),
which were 16 mm apart. Both the samples on the powered electrode and the suspended
samples were flipped over midway through the treatment. For all samples, the treatment
conditions were 100 sccm C
3F
8, 40 mPa (300 mTorr), and 1000 Watts applied RF power.
[0108] Each sample was analyzed for fluorine content in each of the four layers. Exposure
times, sample position during treatment, and results are shown in Table 4.
Table 4
| Sample |
Total time |
Position |
Fluorine Content in ppm |
| |
(sec) |
|
1st Layer |
2nd Layer |
3rd Layer |
4th layer |
| 7-A |
20 |
Suspended |
45 |
Under 5 |
Under 5 |
17 |
| 7-B |
20 |
electrode |
3828 |
1249 |
847 |
2601 |
| 7-C |
120 |
Suspended |
70 |
41 |
40 |
137 |
| 7-D |
120 |
electrode |
9148 |
4732 |
3834 |
6872 |
| 7-E |
240 |
Suspended |
146 |
86 |
95 |
147 |
| 7-F |
240 |
electrode |
10475 |
5539 |
4826 |
7598 |
[0109] As seen in the above table, the concentration of fluorine in each of the four layers
of a sample was substantially more for the samples within an ion sheath than for those
outside the ion sheath.
Example 8
[0110] This example illustrates the effect of a perforated electrode on the plasma treatment.
[0111] Example 8 was made as Example 2 except the grounded electrode had holes with diameters
of 4.8 mm (0.188 inches) and center-to-center spacings of 6.4 mm (0.250 inches), and
the chamber pressure was 67 Pa (500 mTorr). A bright plasma was seen everywhere in
the chamber including the regions on the side of the perforated grounded electrode
opposite the side facing the powered electrode.
[0112] Example 8 was tested for oil repellency. The Oil Repellency Rating was 5. This shows
that a perforated electrode, which allowed the plasma to fill the entire chamber more
easily than with a standard electrode, had no detrimental effect on the properties
of the resulting article.
Example 9 and Comparative Examples 4 and 5
[0113] This example illustrates the influence of electrode spacing on the fluorination of
porous and non-porous substrates at comparable volumetric power densities.
[0114] Samples of Example 9 were made in a manner similar to that of Example 1-D except
the distance between electrodes was varied, and conditions were changed as described
herein. The fluorination treatment was carried out for a treatment time of 10 seconds
with the C
3F
8 gas flow rate maintained at 100 sccm and the chamber pressure maintained at 67 Pa
(0.500 Torr). Samples A and B were flipped over and additionally treated on the backside
of the article for another 10 seconds for a total exposure time of 20 seconds. RF
power was adjusted to nominally maintain the same power density per unit volume of
space between the two electrodes for the different electrode distances. The power
density for Sample A was 0.171 W/cm
3. The power density for Sample B was 0.179 W/cm
3.
[0115] Comparative Examples 4 and 5 were made as in Sample A and B, respectively, except
the substrate for the Comparative Examples was a 0.18 mm thick polycarbonate non-porous
film and the Comparative Examples were not flipped over during plasma treatment, so
the total exposure time was only 10 seconds on one side. The oil repellency of the
untreated non-porous films was 0.
[0116] Samples were tested for oil repellency. The varied process conditions and results
are shown in Table 5.
Table 5
| Sample |
Substrate Type |
Distance (mm) |
Time (sec) |
Power (W) |
Repel. Rating |
| |
|
|
|
|
|
| 9-A |
porous |
16.0 |
20 |
1000 |
5 |
| 9-B |
porous |
28.5 |
20 |
1900 |
2 |
| CE-4 |
non-porous |
16.0 |
10 |
1000 |
6 |
| CE-5 |
non-porous |
28.5 |
10 |
1900 |
6 |
[0117] As seen in Table 5, the results obtained for the porous substrates were drastically
different depending upon the electrode spacing. The porous article made with an electrode
spacing of 16 mm withstood a No.5 fluid in the Oil Repellency Test whereas the porous
article made with an electrode spacing of 28.5 mm withstood only a No. 2 fluid. In
contrast, non-porous samples were not affected by the electrode spacing.
Example 10
[0118] In order to understand the effect of deposition rate of the fluorocarbon on a porous
sample, the treatment conditions used to make Samples 9-A and 9-B were repeated on
Samples 10-A and 10-B, respectively. The substrates for samples 10-A and 10-B were
pieces of silicon over which a polystyrene film had been spin-coated. Portions of
the substrates were masked with tape to allow for step-height measurements using a
stylus profilometer available as Alpha-Step 500 from Tencor Instruments, Mountainview,
CA. The samples were not flipped over. Total exposure time was 120 seconds, chamber
pressure was 67 Pa (500 mTorr) and gas flow rate was 100 sccm. Power was varied as
described above to maintain comparable power densities.
[0119] Samples were tested for oil repellency. The process conditions and deposition rate
results are shown in Table 6.
Table 6
| Sample |
Time (sec) |
Power (W) |
Distance (mm) |
Flow (sccm) |
Deposition Rate (nm/s) |
| 10-A |
120 |
1000 |
16 |
100 |
2.16 |
| 10-B |
120 |
1900 |
28 |
100 |
2.27 |
[0120] The measured deposition rate of 2.16 nanometers/second for sample 10-A was nominally
the same as the rate of 2.27 nanometers/second for sample 10-B. Thus the superior
repellency performance of Sample 9-A over Sample 9-B was not due to a higher deposition
rate and thicker film. This illustrates that the superior article properties provided
by the invention are not due to depositing thicker fluorinated layers, but are due
to more efficient plasma fluorination of article interiors.
Example 11
[0121] This example illustrates the benefit of locating the porous substrate on the powered
electrode for short treatment times.
[0122] Samples for Example 11 were made as in Example 1-D except the electrode separation
distance was 16 mm (0.625 in) and some process conditions were different as described
herein. Sample A was located on the powered electrode whereas sample B was located
on the grounded electrode. Both samples were secured to the electrode with removable
Scotch tape on the edges. Fluorination was done at a chamber pressure of 67 Pa(500
mTorr) with a C
3F
8 flow rate of 100 sccm, and RF power maintained at 1000 W. Both the samples were treated
for 10 seconds, then flipped over and treated on the opposite side for another 10
seconds for a total treatment time of 20 seconds.
[0123] The samples were tested for oil repellency and the results are summarized in Table
7.
Table 7
| Sample |
Substrate Location |
Electrode Spacing (mm) |
Time (sec) |
Power (W) |
Repel. Rating |
| 11-A |
Powered |
16.0 |
20 |
1000 |
5 |
| |
Electrode |
|
|
|
|
| 11-B |
Grounded |
16.0 |
20 |
1000 |
2 |
| |
Electrode |
|
|
|
|
[0124] As seen in the table, the oil repellency rating of the sample located on the powered
electrode was significantly better than the sample located on the grounded electrode.
Example 12
[0125] This example demonstrates the efficacy of the fluorination process when the electrode
spacing is less than 12 mm (0.5 in). Stable plasma operation is generally not possible
with such a small spacing. By operating the C
3F
8 plasma at a pressure of 67 Pa (500 mTorr) and power of 1000 Watts, a surprisingly
stable plasma was obtained even when the electrode spacing was as low as 6.3 mm (0.25
in). Samples for Example 12 were made as in Example 1-D except the electrode separation
distance was 8.6 mm (0.340 in) for sample 12-A and 6.3 mm (0.25 in) for samples 12-B
and 12-C. Fluorination was done at a chamber pressure of 67 Pa (500 mTorr) with a
C
3F
8 flow rate of 100 sccm, and RF power maintained at 1000 W. Samples 12-A and 12-B were
treated for 10 seconds, then flipped over and treated on the opposite side for another
10 seconds for a total treatment time of 20 seconds. Sample 12-C was treated in the
same manner using the same process conditions but the treatment time was for 5 seconds
per side, a total treatment time of 10 seconds. The Oil Repellency Ratings of these
samples are summarized in Table 8.
Table 8
| Sample |
Substrate Location |
Electrode Spacing (mm) |
Time (sec) |
Power (W) |
Repel. Rating |
| 12-A |
Powered |
8.6 |
20 |
1000 |
5 |
| |
Electrode |
|
|
|
|
| 12-B, |
Powered |
6.3 |
20 |
1000 |
5 |
| |
Electrode |
|
|
|
|
| 12-C |
Powered |
6.3 |
10 |
1000 |
5 |
| |
Electrode |
|
|
|
|
As can be seen from the data, the Repellency Rating is excellent even when the treatment
times are as small as 10 seconds.
Example 13
[0126] This example demonstrates the effect of treating a porous article on the grounded
electrode with a small electrode spacing.
[0127] Samples of the web described in Example 1 were plasma fluorinated at a C
3F
8 flow rate of 83 sccm, a chamber pressure of 40 Pa (300 mTorr), RF power maintained
at 1000 Watts, and an electrode spacing of 16 mm. Sample 13-A was placed in the ion
sheath adjacent to the powered electrode while sample 13-B was placed in the ion sheath
adj acent to the grounded electrode. The samples were hydrocharged and tested for
DOP penetration using the standard test method. Q
200 for Example 13-A was 1.24. Q
200 for Example 13-B was 1.06.
1. Verfahren zum Fluorieren eines porösen Artikels, Folgendes umfassend:
Bereitstellen einer Reaktionskammer mit einem kapazitiv gekoppelten System, das mindestens
eine geerdete Elektrode und mindestens eine, von einer RF-Quelle gespeiste Elektrode
umfasst,
Erzeugen eines Fluor enthaltenden Plasmas in der Kammer, womit die Bildung einer Ionenhülle
um die Elektroden bewirkt wird,
Anordnen eines porösen Artikels in der Ionenhülle der gespeisten Elektrode und
Reagierenlassen von reaktionsfähigen Spezies des Plasmas mit der Oberfläche und dem
Inneren des Artikels,
wodurch der Artikel fluoriert wird.
2. Verfahren zum Fluorieren eines porösen Artikels, Folgendes umfassend:
Bereitstellen einer Reaktionskammer mit einem kapazitiv gekoppelten System, das mindestens
eine, von einer RF-Quelle gespeiste Elektrode und mindestens eine geerdete Elektrode
umfasst, die im Wesentlichen parallel zur Fläche der gespeisten Elektrode liegt und
von der geerdeten Elektrode 25 Millimeter oder weniger entfernt ist,
Erzeugen eines Fluor enthaltenden Plasmas in der Kammer bei einem Druck von etwa 40
Pascal oder weniger,
Anordnen eines porösen Artikels zwischen den im Wesentlichen parallelen Elektroden
und außerhalb einer gegebenenfalls vorhandenen Ionenhülle und
Reagierenlassen von reaktionsfähigen Spezies des Plasmas mit der Oberfläche und dem
Inneren des Artikels über eine Gesamtbehandlungszeit von über zwei Minuten
wodurch der Artikel fluoriert wird.
3. Verfahren zum Fluorieren eines porösen Artikels, Folgendes umfassend:
Bereitstellen einer Reaktionskammer mit einem kapazitiv gekoppelten System, das mindestens
eine, von einer RF-Quelle gespeiste Elektrode und mindestens eine geerdete Elektrode
umfasst, die im Wesentlichen parallel zur Fläche der gespeisten Elektrode liegt und
von der geerdeten Elektrode 25 Millimeter oder weniger entfernt ist,
Erzeugen eines Fluor enthaltenden Plasmas in der Kammer, womit die Bildung einer Ionenhülle
um die Elektroden bewirkt wird,
Anordnen eines porösen Artikels in der Ionenhülle der geerdeten Elektrode und
Reagierenlassen von reaktionsfähigen Spezies des Plasmas mit der Oberfläche und dem
Inneren des Artikels über eine Gesamtbehandlungszeit von etwa 30 Sekunden bis etwa
5 Minuten
wodurch der Artikel fluoriert wird.
4. Verfahren zum Fluorieren eines porösen Artikels, Folgendes umfassend:
Bereitstellen einer Reaktionskammer mit einem kapazitiv gekoppelten System, das mindestens
eine, von einer RF-Quelle gespeiste Elektrode und mindestens eine geerdete Elektrode
umfasst, die im Wesentlichen parallel zur Fläche der gespeisten Elektrode liegt und
von der geerdeten Elektrode 13 Millimeter oder weniger entfernt ist,
Erzeugen eines Fluor enthaltenden Plasmas in der Kammer, womit die Bildung einer Ionenhülle
um die Elektroden bewirkt wird,
Anordnen eines porösen Artikels zwischen den Elektroden und
Reagierenlassen von reaktionsfähigen Spezies des Plasmas mit der Oberfläche und dem
Inneren des Artikels,
wodurch der Artikel fluoriert wird.
5. Verfahren nach Anspruch 1, wobei der Artikel Poren aufweist, die kleiner als die mittlere
freie Weglänge jeglicher Spezies in dem Plasma sind.
6. Verfahren nach Anspruch 1, wobei der Vorgang kontinuierlich ist.
7. Verfahren nach Anspruch 1, wobei die Behandlungszeit weniger als etwa 60 Sekunden
beträgt.
8. Verfahren nach Anspruch 1, wobei der poröse Artikel aus der Gruppe ausgewählt ist,
die aus Schäumen, gewebten Materialien, nicht gewebten Materialien, Membranen, Fritten,
porösen Fasern, Textilien und mikroporösen Artikeln besteht.
9. Verfahren nach Anspruch 1, wobei der Artikel zwei parallele Hauptflächen aufweist
und auf einer Hauptfläche behandelt wird.
10. Verfahren nach Anspruch 9, wobei der Artikel ferner auf seiner zweiten Hauptfläche
behandelt wird.
11. Verfahren nach Anspruch 1, wobei die Elektroden 25 Millimeter oder weniger voneinander
entfernt sind.
12. Verfahren nach Anspruch 1, wobei die Elektroden 16 Millimeter oder weniger voneinander
entfernt sind.
13. Vorrichtung zum Fluorieren eines Substrats, Folgendes umfassend:
eine Vakuumkammer,
ein kapazitiv gekoppeltes System innerhalb der Kammer, das mindestens eine, von einer
RF-Quelle gespeiste Elektrode und mindestens eine geerdete Elektrode, die im Wesentlichen
parallel zur gespeisten Elektrode liegt, umfasst, wobei die Elektroden 25 Millimeter
oder weniger voneinander entfernt sind, und
ein Mittel zum Erzeugen eines Fluor enthaltenden Plasmas in der gesamten Kammer.
14. Vorrichtung nach Anspruch 13, wobei die Elektroden 16 Millimeter oder weniger voneinander
entfernt sind.
15. Vorrichtung nach Anspruch 13, wobei die gespeiste Elektrode eine rotierende Walze
ist.
16. Vorrichtung nach Anspruch 15, die ferner eine zweite gespeiste Elektrode in Form einer
rotierenden Walze umfasst.
17. Vorrichtung nach Anspruch 13, wobei das kapazitiv gekoppelte System einen asymmetrischen
Parallelplattenreaktor umfasst.